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The dynamic resistance of the tunnel diode in the high voltage state is low, but not | The dynamic resistance of the tunnel diode in the high voltage state is low, but not | ||
low enough for the diode to be modeled as a rock-solid voltage source. | low enough for the diode to be modeled as a rock-solid voltage source. | ||
It is approximated by | It is approximated in theory by | ||
* r_d = 0.025V / 0.006 = 4.2 ohms | * r_d = 0.025V / 0.006 = 4.2 ohms | ||
Empirical measurements were closer to 7 ohms. | |||
the tunnel diode | This, plus the 43-ohm output resistor, | ||
makes for a 50-ohm output resistance when the tunnel diode is in | |||
the high-voltage state. To prevent the 43 ohm output resistor from | |||
appearing inductive and spoiling the flat top of the output waveform, | |||
the resistor is actually | |||
mounted inside the BNC output connector. The center | |||
conductor of the connector has a small hole to accept the 43 ohm | |||
resistor’s lead. Because of this, the resonant frequency of the | |||
TD and its parasitics is around 3GHz and well damped. | |||
For any scope with less than about 1.5GHz BW, the ring would | |||
likely be invisible. | |||
* [http://w140.com/tek_067-0681-01.pdf Tektronix 067-0681-01 Datasheet (PDF)] | * [http://w140.com/tek_067-0681-01.pdf Tektronix 067-0681-01 Datasheet (PDF)] |